新甘交界红柳河地区二叠纪玄武岩年代学、地球化学及构造意义   总被引：8，自引：4，他引：4  

潘金花  郭召杰  刘畅  赵泽辉 《岩石学报》2008,24(4)

新甘交界红柳河地区二叠系剖面中发育有块状和枕状玄武岩,激光ArAr定年确定的玄武岩形成时间在280～300Ma之间;玄武岩SiO_2含量为44.71%～49.27%,Mg~#为42.4～52.4,(~(87)Sr/~(86)Sr)_i为0.703834～0.706819,(~(143)Nd/~(144)Nd)_i为0.518861～0.5121220,ε_(Nd)(t)为-3.01～3.67。玄武岩微量元素、稀土元素和Sr-Nd同位素均显示出与OIB性质相似的特征。其弱富集的不相容元素和轻稀土元素,显示出源区富集的特点。而Zr/Nb(14.63)和Th/U(2.83)则指示岩浆中可能有少量循环原始地幔和亏损地幔物质的加入。综合对比北山南部柳园地区二叠纪玄武岩源区特征,提出红柳河地区早二叠世OIB型玄武岩主要来源于北山地区晚古生代裂谷带下伏已被不同程度改造的富集地幔。  相似文献   

安徽铜陵朝山金矿床流体包裹体研究   总被引：3，自引：1，他引：2  

杨小男  徐兆文  高庚  陆现彩  刘苏明  李海勇 《岩石学报》2008,24(8)

朝山金矿床是狮子山矿田内的热液交代型金矿床,在成因上与燕山期的白芒山辉石闪长岩有关.通过采集发育在不同深度下的含金黄铁矿-石英一方解石脉样品,进行流体包裹体岩相学观察和显微测温发现,石英和方解石中均捕获了富气相、富液相的两相水溶液包裹体和含子晶的三相水溶液包裹体,以上三种类型包裹体的均一温度统计峰值分别出现于315～335℃和255～275℃,盐度的统计峰值出现于17.50%～22.50%NaCl eq.和32.50%～37.50%NaCl eq.之间.激光拉曼探针分析表明,石英中流体包裹体的气相成分以水蒸汽为主,伴有少量CO2,可能含有CH4.流体的H、O同位素组成具确岩浆水特征.上述研究表明.朝山金矿成矿流体经历了相态变化,发生了不均匀捕获.受燕山期岩浆作用影响,狮子山矿田内的铜、金成矿在时空上具有一定联系,成矿流体运移的过程中,主要发生了相分离、气相液化和减压沸腾作用,可能是形威铜、金矿化分带的重要原因.  相似文献   

氮气、氧气和空气水合物的合成及其拉曼光谱特征   总被引：1，自引：0，他引：1  

刘昌岭  业渝光  卢海龙 《现代地质》2008,22(3):480-484

在-20℃和不同的压力下,在实验室内分别合成了氮气水合物(16MPa)、氧气水合物(13MPa)和空气水合物(15MPa),并对其N—N和O—O键伸缩振动的拉曼光谱特征进行了研究。结果表明,人工合成的水合物中的N—N和O—O键的拉曼位移与天然的空气水合物中的数据十分接近。在氮气水合物和空气水合物中,N—N键的拉曼峰值均为2322.4cm-1;O—O键的拉曼峰值在氧气水合物和空气水合物保持一致,均为1547.8cm-1。空气水合物分解的拉曼谱图表明,它不是氮气水合物和氧气水合物组成的混合物,而是由氮分子和氧分子共同生成的单一水合物,氮分子和氧分子同时进入水合物的大笼和小笼中。与空气中的氮、氧比例相比,水合物中氧分子明显富集,氮分子和氧分子的比例为2.4∶1。  相似文献   

Laser ablation coupled with ICP-MS applied to U–Pb zircon geochronology: A review of recent advances   总被引：2，自引：2，他引：0  

Alain Cocherie  Michle Robert 《Gondwana Research》2008,14(4):597

Improvements in the technology of laser ablation and ICP-MS instruments make LA-MC-ICPMS a rapid, precise and accurate method for U–Pb zircon geochronology. In this review we describe the main stages of the evolution of this in situ approach from the early 1990s to the present time. Some key points have been progressively improved. The crater size has been reduced to achieve real in situ measurements. The laser wavelength has been reduced as well as the duration of each pulse in order to lower inter-element fractionation. The blank from the gas has to be lowered as far as possible. Double focusing instruments and magnetic field sectors allow flat-topped peaks required for precise isotope ratio measurement to be obtained. The use of a multi-ion counting system significantly improves the sensitivity of the method and the static mode of integration favours the precision of measurement of the transient signal originating from a noisy laser ablated particle beam.Combining the use of a 213 nm UV laser and a MC-ICPMS equipped with a multi-ion counting system operating in static mode, the common precisions achieved for the key ratios ²⁰⁷Pb/²⁰⁶Pb and ²⁰⁶Pb/²³⁸U are better than 1% and 3% (2σ) respectively, including error propagation associated with standard normalization. Until now, the use of a zircon standard has remained necessary to ensure the accuracy of the calculated age. A strategy for common-Pb correction is proposed according to the age of the zircon and according to the Th/U ratio of the grains. After recording sixteen to twenty spot analyses the precision usually achieved on the age is about 1% and even significantly better for Proterozoic samples.In order to show the performance achieved by modern LA-MC-ICPMS geochronology, we tested four zircon samples covering a wide age range from 290 to 2440 Ma. These new age determinations can be compared in term of precision and accuracy since they have already been dated by reference methods (ID-TIMS and SHRIMP). Further developments in the technology of ion counters equipping modern MC-ICPMS and in laser systems will certainly be applied to a large field of geochronology studies in the near future as an alternative to SIMS for in situ age determination.  相似文献   

Laser probe Ar/Ar dating: History and development from a technical perspective     

Hironobu Hyodo   《Gondwana Research》2008,14(4):609

The ⁴⁰Ar/³⁹Ar method using a laser probe opened the door to microscale measurements and diffusion profiles frozen in samples. In the first decade since the initial application of a laser for ⁴⁰Ar/³⁹Ar dating in 1973, practical applications have been few. This is due not only to the fact that the laser and vacuum technologies were immature but that mass spectrometry was also in its infancy. In those days, the sensitivity of a mass spectrometer was generally insufficient to measure the small amount of argon degassed from a geological sample by a laser. These problems have subsequently been solved by new technologies. To understand their current status, a brief history of their development is outlined. This outline focuses on the required detection limit in micro scale measurement, practical approaches for accurate measurement are explained through examples in our laboratory specifically relating to the technical aspects of ⁴⁰Ar/³⁹Ar dating.  相似文献   

山东玲珑金矿床成矿流体地球化学特征   总被引：3，自引：0，他引：3  

王可勇  张春燕  樊岳铭  张晓东 《吉林大学学报(地球科学版)》2008,38(2):194-201

玲珑金矿床第一成矿阶段与含金黄铁矿共生的石英中主要发育4种类型的原生流体包裹体:Ⅰ气液两相,Ⅱ含CO2三相,ⅢCO2,Ⅳ单液相包裹体。流体包裹体成分激光拉曼光谱分析及测温结果显示:①Ⅰa型包体,气液比10%~15%,均一温度为162.7~235.6℃,w(NaCl)(盐度)为4.65%~7.59%,气相平均摩尔分数为:H2O 96.48%,CO22.4%;②Ⅰb型包体,气液比30%~45%,均一温度266.9~349.2℃,w(NaCl)为10.8%~13.4%,气相平均摩尔分数为H2O 69.75%,CO224.74%;③Ⅱ型含CO2包体,CO2相所占比例为20%~90%,其均一温度为193.5~321.6℃,w(NaCl)2.9%~5.3%,CO2相中,H2O的摩尔分数为27.72%,CO2为70.6%。包裹体成分分析及测温结果综合研究认为,玲珑金矿成矿过程中存在大气降水热液与地幔来源流体的混合作用,前者与从流体中分离出的富CO2流体混合,以不同比例被捕获形成Ⅱ型包体;而与分异出CO2后的CO2不饱和地幔流体混合,被捕获形成Ⅰb型包体。两种流体混合导致的含矿热液物化条件变化对金的沉淀成矿具有重要意义。  相似文献   

笼状水合物拉曼光谱特征与结构水合数的耦合关系   总被引：3，自引：0，他引：3  

雷怀彦  官宝聪  刘建辉  李震 《现代地质》2005,19(1):83-88

为了探讨不同气体组分和环境介质对形成笼状结构类型水合物和水合数的影响, 开展了一元体系 (CH4、CO2、C3H8 )和二元体系(CH4 +CO2、CH4 +C3H8、CH4 +N2 )的水合物生成结晶充填过程、结晶构型和动力学特性分析, 并对生成的水合物进行了拉曼光谱分析。结果表明单组分甲烷充填小孔穴 512和大孔穴 512 62 形成Ⅰ型笼状结构水合物(SⅠ), 二氧化碳和丙烷只占据大孔穴 512 64 形成Ⅱ型笼状结构水合物 (SⅡ ); 而二元混合组分中小孔穴中只充填有甲烷, 而没有CO2、N2 和C3H8。应用反褶积的ν1 对称谱带测定了CH4 分子在Ⅰ型结构大孔穴和小孔穴中的相对占有率,并根据谱带的面积比(对应于小孔穴与大孔穴)计算了平衡条件下甲烷水合物孔穴占有率及其耦合的水合数, 认为气体分子的大小不仅影响它所充填的孔穴形态和类型, 而且影响水合物生成的结构类型和水合数。  相似文献   

大别山及苏鲁地区微粒金刚石分类及其大地构造意义   总被引：3，自引：1，他引：3  

徐树桐  刘贻灿  陈冠宝  季寿元  倪培  萧万生 《地质通报》2005,24(12):1081-1088

1992年发现大别山首例微粒金刚石之后，又于2003年和2004年在大别山和苏鲁地区的榴辉岩薄片中和榴辉岩的人工重砂中发现了微粒金刚石。本文报道其中尚未发表的7颗，并对2颗较大的薄片中的微粒金刚石和2颗自由晶体金刚石进行拉曼光谱和红外光谱测试。研究结果表明，本区所有微粒金刚石都为IaA和IaB型金刚石的混合体。缺少Ib型金刚石，表明没有人造金刚石的混入。薄片中的金刚石大部分为石榴子石的包裹体，少数产出于颗粒之间，直径为30-180μm。自由颗粒微粒金刚石直径为400-700μm。在大别山北部，不但又一次找到了微粒金刚石，还在石榴子石中发现有单斜辉石、磷灰石和金红石的出溶。这表明北大剐不但是超高压地质体，而且可能是本区俯冲最深的地质体。  相似文献   

Effects of laser beam alignment tolerance on lidar accuracy   总被引：2，自引：0，他引：2  

Damir Latypov   《ISPRS Journal of Photogrammetry and Remote Sensing》2005,59(6):361-368

One of the major lidar error sources not yet analyzed in the literature is the tolerance of the laser beam alignment with respect to the scanning mirror. In this paper, the problem of quantifying these errors is solved for rotating polygon mirror type lidar systems. An arbitrary deviation of the beam from its design direction–the vector of beam misalignment–can be described by two independent parameters. We choose these as horizontal and vertical components of the misalignment vector in the body frame. Either component affects both, horizontal and vertical lidar accuracy. Horizontal lidar errors appear as scan line distortions—along and across track shifts, rotations and scaling. It is shown that the horizontal component of misalignment results in a scan line first being shifted across the track and then rotated around the vertical at the new center of the scan line. Resulting vertical lidar error, being a linear function of the scan angle, is similar to that produced by a roll bias. The vertical component of the beam misalignment causes scan line scaling and an along track shift. The corresponding vertical error is quadratic with respect to the scan angle. The magnitude of these effects is significant even at tight alignment tolerances and cannot be realistically accounted for in the conventional calibration model, which includes only range, attitude and GPS biases. Therefore, in order to attain better accuracy, this model must be expanded to include the beam misalignment parameters as well. Addition of new parameters into the model raises a question of whether they can be reliably solved for. To give a positive answer to this question, a calibration method must utilize not only ground control information, which is typically very limited, but also the relative accuracy information from the overlapping flight lines.  相似文献   

Isothermal annealing of partially metamict zircon: evidence for a three-stage recovery process     

T. Geisler 《Physics and Chemistry of Minerals》2002,29(6):420-429

 Raman spectroscopy and the powder diffraction technique have been used to monitor the recovery process of two partially metamict zircons (2.6 and 4.8 × 10¹⁸ α-decays g⁻¹) from Sri Lanka during a series of isothermal annealing experiments in the temperature range from 870 to 1622 K. These experiments show for the first time that structural recovery in partially metamict zircon proceeds via three distinct recovery stages, each of which occurs within a distinct time-temperature regime. Whereas the first two stages have previously been recognized (recovery of damaged crystalline remnants and epitaxial recrystallization), the third stage has not yet been identified as a single activated process. It is suggested that anisotropic defect annealing during the first stage at low temperatures, where the structure recovers preferentially along the a(b) plane, produces a geometrical situation where large structural rearrangements are necessary to remove the remaining defects inside the crystalline material. This situation is approximately reached when the amorphous domains start to recrystallize. The reason for anisotropic annealing can be found in a different connectivity between polyhedral linkages in both directions of the zircon lattice. High apparent activation energies, in the range of 6.4 to 7.9 eV, were determined for the third recovery stage from the Raman data, which are interpreted to reflect large structural rearrangements (i.e. polyhedral tilting) associated with the final recovery of the c axis. This explains the occurrence of a distinct recrystallization stage without defect annealing. Finally, it should be mentioned that the first recovery stage is not necessarily expected to occur in less damaged zircon crystals (<∼2 × 10¹⁸ α-decays g⁻¹), since less stable defects along the basal plane might have already been self-annealed during radiation damage accumulation under ambient temperatures. Received: 6 September 2001 / Accepted: 25 February 2002  相似文献